Wireless power transmission for electronic devices

ABSTRACT

Exemplary embodiments are directed to wireless power transfer. A wireless power receiver includes a receive antenna for coupling with a transmit antenna of transmitter generating a magnetic near field. The receive antenna receives wireless power from the magnetic near field and includes a resonant tank and a parasitic resonant tank wirelessly coupled to the resonant tank. A wireless power transmitter includes a transmit antenna for coupling with a receive antenna of a receiver. The transmit antenna generates a magnetic near field for transmission of wireless power and includes a resonant tank and a parasitic resonant tank coupled to the resonant tank.

CLAIM OF PRIORITY UNDER 35 U.S.C. §119

This application claims priority under 35 U.S.C. §119(e) to:

-   -   U.S. Provisional Patent Application 61/084,246 entitled        “WIRELESS POWERING & CHARGING” filed on Jul. 28, 2008, the        disclosure of which is hereby incorporated by reference in its        entirety.

BACKGROUND

Typically, each battery powered device such as a wireless electronicdevice requires its own charger and power source, which is usually analternating current (AC) power outlet. Such a wired configurationbecomes unwieldy when many devices need charging.

Approaches are being developed that use over-the-air or wireless powertransmission between a transmitter and a receiver coupled to theelectronic device to be charged. Such approaches generally fall into twocategories. One is based on the coupling of plane wave radiation (alsocalled far-field radiation) between a transmit antenna and a receiveantenna on the device to be charged. The receive antenna collects theradiated power and rectifies it for charging the battery. Antennas aregenerally of resonant length in order to improve the radiation orreceiving efficiency. This approach suffers from the fact that the powercoupling falls off quickly with distance between the antennas. Socharging over reasonable distances (e.g., in the range of 0.5 to 2meters) becomes inefficient. Additionally, since the transmitting systemradiates plane waves, unintentional radiation can interfere with othersystems if not properly controlled through filtering.

Other approaches to wireless energy transmission are based on inductivecoupling between a transmit antenna embedded, for example, in a“charging mat” or surface and a receive antenna (and a rectifyingcircuit) embedded in the host electronic device to be charged. Thisapproach has the disadvantage that the spacing between transmit andreceive antennas must be very close (e.g., within several centimeters).Though this approach does have the capability to simultaneously chargemultiple devices in the same area, this area is typically very small andrequires the user to accurately locate the devices to a specific area.Therefore, there is a need to provide a wireless charging arrangementthat accommodates flexible placement and orientation of transmit andreceive antennas.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 illustrates a simplified block diagram of a wireless powertransmission system.

FIG. 2 illustrates a simplified schematic diagram of a wireless powertransmission system.

FIG. 3 illustrates a schematic diagram of a loop antenna, in accordancewith exemplary embodiments.

FIGS. 4A-4C illustrate a physical implementation of a wireless powertransmission system including a transmitter and receiver, in accordancewith exemplary embodiments.

FIGS. 5A-5B illustrate a physical implementation of a transmitter,energy relay and receiver, in accordance with exemplary embodiments.

FIG. 6 illustrates a device configured to receive wirelessly transmittedpower and to transmit wireless power, in accordance with an exemplaryembodiment.

FIG. 7 illustrates a wired power transmission system.

FIG. 8 illustrates a functional block diagram of a wireless powertransmission system, in accordance with various exemplary embodiments.

FIG. 9 illustrates a circuit diagram of a first coupling variant betweentransmit and receive antennas, in accordance with an exemplaryembodiment.

FIG. 10 illustrates a circuit diagram of a second coupling variantbetween transmit and receive antennas, in accordance with an exemplaryembodiment.

FIG. 11 illustrates a circuit diagram of a third coupling variantbetween transmit and receive antennas, in accordance with an exemplaryembodiment.

FIG. 12 illustrates a circuit diagram of a fourth coupling variantbetween transmit and receive antennas, in accordance with an exemplaryembodiment.

FIG. 13 illustrates a circuit diagram of a fifth coupling variantbetween transmit and receive antennas, in accordance with an exemplaryembodiment.

FIG. 14 illustrates a low frequency/high frequency (LF-HF) transmitter,in accordance with an exemplary embodiment.

FIGS. 15A-15C illustrate various configurations of multiple stagetransmit power conversion units, in accordance with exemplaryembodiments.

FIGS. 16A-16D illustrate various configurations of single stage transmitpower conversion units, in accordance with exemplary embodiments.

FIG. 17 illustrates an LF-HF receiver, in accordance with an exemplaryembodiment.

FIGS. 18A-18H illustrate various configurations of a receive powerconversion unit, in accordance with various exemplary embodiments.

FIG. 19 illustrates a flowchart of a method for receiving wirelesspower, in accordance with an exemplary embodiment.

FIG. 20 illustrates a flowchart of a method for transmitting wirelesspower, in accordance with an exemplary embodiment.

DETAILED DESCRIPTION

The word “exemplary” is used herein to mean “serving as an example,instance, or illustration.” Any embodiment described herein as“exemplary” is not necessarily to be construed as preferred oradvantageous over other embodiments.

The detailed description set forth below in connection with the appendeddrawings is intended as a description of exemplary embodiments of thepresent invention and is not intended to represent the only embodimentsin which the present invention can be practiced. The term “exemplary”used throughout this description means “serving as an example, instance,or illustration,” and should not necessarily be construed as preferredor advantageous over other exemplary embodiments. The detaileddescription includes specific details for the purpose of providing athorough understanding of the exemplary embodiments of the invention. Itwill be apparent to those skilled in the art that the exemplaryembodiments of the invention may be practiced without these specificdetails. In some instances, well-known structures and devices are shownin block diagram form in order to avoid obscuring the novelty of theexemplary embodiments presented herein.

The words “wireless power” are used herein to mean any form of energyassociated with electric fields, magnetic fields, electromagneticfields, or otherwise that is transmitted between a transmitter to areceiver without the use of physical electromagnetic conductors. Powerconversion in a system is described herein to wirelessly charge devicesincluding, for example, mobile phones, cordless phones, iPod, MP3players, headsets, etc. Generally, one underlying principle of wirelessenergy transfer includes magnetic coupled resonance (i.e., resonantinduction) using frequencies, for example, below 30 MHz. However,various frequencies may be employed including frequencies wherelicense-exempt operation at relatively high radiation levels ispermitted, for example, at either below 135 kHz (LF) or at 13.56 MHz(HF). At these frequencies normally used by Radio FrequencyIdentification (RFID) systems, systems must comply interference andsafety standards such as EN 300330 in Europe or FCC Part 15 norm in theUnited States. By way of illustration and not limitation, theabbreviations LF and HF are used herein where “LF” refers to f₀=135 kHzand “HF” to refers to f₀=13.56 MHz.

FIG. 1 illustrates wireless power transmission system 100, in accordancewith various exemplary embodiments. Input power 102 is provided to atransmitter 104 for generating a magnetic field 106 for providing energytransfer. A receiver 108 couples to the magnetic field 106 and generatesan output power 110 for storing or consumption by a device (not shown)coupled to the output power 110. Both the transmitter 104 and thereceiver 108 are separated by a distance 112. In one exemplaryembodiment, transmitter 104 and receiver 108 are configured according toa mutual resonant relationship and when the resonant frequency ofreceiver 108 and the resonant frequency of transmitter 104 are matched,transmission losses between the transmitter 104 and the receiver 108 areminimal when the receiver 108 is located in the “near-field” of themagnetic field 106.

Transmitter 104 further includes a transmit antenna 114 for providing ameans for energy transmission and receiver 108 further includes areceive antenna 118 for providing a means for energy reception. Thetransmit and receive antennas are sized according to applications anddevices to be associated therewith. As stated, an efficient energytransfer occurs by coupling a large portion of the energy in thenear-field of the transmitting antenna to a receiving antenna ratherthan propagating most of the energy in an electromagnetic wave to thefar field. In this near-field, a coupling may be established between thetransmit antenna 114 and the receive antenna 118. The area around theantennas 114 and 118 where this near-field coupling may occur isreferred to herein as a coupling-mode region.

FIG. 2 shows a simplified schematic diagram of a wireless powertransmission system. The transmitter 104 driven by input power 102includes an oscillator 122, a power amplifier 124 and a filter andmatching circuit 126. The oscillator is configured to generate a desiredfrequency, which may be adjusted in response to adjustment signal 123.The oscillator signal may be amplified by the power amplifier 124 withan amplification amount responsive to control signal 125. The filter andmatching circuit 126 may be included to filter out harmonics or otherunwanted frequencies and match the impedance of the transmitter 104 tothe transmit antenna 114.

The receiver 108 may include a matching circuit 132 and a rectifier andswitching circuit 134 to generate a DC power output to charge a battery136 as shown in FIG. 2 or power a device coupled to the receiver (notshown). The matching circuit 132 may be included to match the impedanceof the receiver 108 to the receive antenna 118.

As illustrated in FIG. 3, antennas used in exemplary embodiments may beconfigured as a “loop” antenna 150, which may also be referred to hereinas a “magnetic” or “resonant” antenna. Loop antennas may be configuredto include an air core or a physical core such as a ferrite core.Furthermore, an air core loop antenna allows the placement of othercomponents within the core area. In addition, an air core loop may morereadily enable placement of the receive antenna 118 (FIG. 2) within aplane of the transmit antenna 114 (FIG. 2) where the coupled-mode regionof the transmit antenna 114 (FIG. 2) may be more effective.

As stated, efficient transfer of energy between the transmitter 104 andreceiver 108 occurs during matched or nearly matched resonance betweenthe transmitter 104 and the receiver 108. However, even when resonancebetween the transmitter 104 and receiver 108 are not matched, energy maybe transferred at a lower efficiency. Transfer of energy occurs bycoupling energy from the near-field of the transmitting antenna to thereceiving antenna residing in the neighborhood where this near-field isestablished rather than propagating the energy from the transmittingantenna into free space.

The resonant frequency of the loop or magnetic antennas is based on theinductance and capacitance. Inductance in a loop antenna is generallythe inductance created by the loop, whereas, capacitance is generallyadded to the loop antenna's inductance to create a resonant structure ata desired resonant frequency. As a non-limiting example, capacitor 152and capacitor 154 may be added to the antenna to create a resonantcircuit that generates a sinusoidal or quasi-sinusoidal signal 156.Accordingly, for larger diameter loop antennas, the size of capacitanceneeded to induce resonance decreases as the diameter or inductance ofthe loop increases. Furthermore, as the diameter of the loop or magneticantenna increases, the efficient energy transfer area of the near-fieldincreases for “vicinity” coupled devices. Of course, other resonantcircuits are possible. As another non-limiting example, a capacitor maybe placed in parallel between the two terminals of the loop antenna. Inaddition, those of ordinary skill in the art will recognize that fortransmit antennas the resonant signal 156 may be an input to the loopantenna 150.

Exemplary embodiments of the invention include coupling power betweentwo antennas that are in the near-fields of each other. As stated, thenear-field is an area around the antenna in which electromagnetic fieldsexist but may not propagate or radiate away from the antenna. They aretypically confined to a volume that is near the physical volume of theantenna. In the exemplary embodiments of the invention, magnetic typeantennas such as single and multi-turn loop antennas are used for bothtransmit (Tx) and receive (Rx) antenna systems since most of theenvironment possibly surrounding the antennas is dielectric and thus hasless influence on a magnetic field compared to an electric field.Furthermore, “electric” antennas (e.g., dipoles and monopoles) or acombination of magnetic and electric antennas is also contemplated.

The Tx antenna can be operated at a frequency that is low enough andwith an antenna size that is large enough to achieve good couplingefficiency (e.g., >10%) to a small Rx antenna at significantly largerdistances than allowed by far field and inductive approaches mentionedearlier. If the Tx antenna is sized correctly, high couplingefficiencies (e.g., 30%) can be achieved when the Rx antenna on a hostdevice is placed within a coupling-mode region (i.e., in the near-field)of the driven Tx loop antenna

The various exemplary embodiments disclosed herein identify differentcoupling variants which are based on different power conversionapproaches, and the transmission range including device positioningflexibility (e.g., close “proximity” coupling for charging pad solutionsat virtually zero distance or “vicinity” coupling for short rangewireless power solutions). Close proximity coupling applications(strongly coupled regime, coupling factor typically k>0.1) provideenergy transfer over short or very short distances typically in theorder of Millimeters or Centimeters depending on the size of theantennas. Vicinity coupling applications (loosely coupled regime,coupling factor typically k<0.1) provide energy transfer at relativelylow efficiency over distances typically in the range from 10 cm to 2 mdepending on the size of the antennas.

As described herein, “proximity” coupling and “vicinity” coupling may beconsidered as different methods of matching the power source/sink to theantenna/coupling network. Moreover, the various exemplary embodimentsprovide system parameters, design targets, implementation variants, andspecifications for both LF and HF applications and for the transmitterand receiver. Some of these parameters and specifications may vary, asrequired for example, to better match with a specific power conversionapproach. System design parameters may include various priorities andtradeoffs. Specifically, transmitter and receiver subsystemconsiderations may include high transmission efficiency, low complexityof circuitry resulting in a low-cost implementation.

FIGS. 4A-4C illustrate a physical implementation of a wireless powertransmission system including a transmitter and receiver, in accordancewith exemplary embodiments. In one exemplary embodiment of FIG. 4A, atransmitter may be configured within a Single Device Charging Pad (SDCP)200 including a transmit antenna 202. SDCP 200 may also be scalable andextended to a multiple device charging pad 204 including transmitantenna 206 and transmit antenna 208, illustrated in FIG. 4A to includea plurality of SDCPs. FIG. 4B illustrates an SDCP 200 including atransmit antenna (not shown) coupling with a device (e.g., cellphone,PDA, MP3 player, etc.) including a receive antenna (not shown) forreceiving wirelessly transferred power at a device 210. FIG. 4B alsoillustrates a multiple device charging pad 204 including a firsttransmit antenna (not shown) and a second transmit antenna (not shown)for respectively charging device 212 and device 214. Similarly, FIG. 4Cillustrates an SDCP 200 including a transmit antenna (not shown)coupling with another form factor micro device 216 (e.g., wirelessheadset, etc.) including a receive antenna (not shown) for receivingwirelessly transferred power at device 216. FIG. 4C also illustrates amultiple device charging pad 204 including a first transmit antenna (notshown) and a second transmit antenna (not shown) for respectivelycharging device 218 and device 220.

SDCPs may be variously configured and variously capable, by way ofexample and not limitation, an SDCP may be configured for highefficiency charging for medium size devices requiring a charging powerin the order of 4 Watts. Alternatively, an SDCP may be configured formedium efficiency charging for small form factor very low power devicessuch as headsets, MP3 players, etc. requiring a charging power below 1Watt.

FIGS. 5A-5B illustrate a physical implementation of a wireless powertransmission system including a transmitter, energy relay and receiver,in accordance with exemplary embodiments. Wireless power transfer may beextended using a parasitic resonant antenna, also known as an “energyrelay” coil/antenna/loop or “repeater” coil/antenna/loop. While“vicinity” coupling between a transmitter and receiver may not providehigh efficiency energy transfer, “vicinity” coupling providesflexibility in positioning of the receiver (with the device attachedthereto) with respect to the transmitter antenna.

FIG. 5A illustrates a configuration of wireless power transmissionsystem including an intermediate energy relay, in accordance with anexemplary embodiment. A wireless power transmission system 250 includesa transmitter 252 illustrated as a SDCP. The transmitter 252 furtherincludes a transmit antenna 254 and the transmitter 252 receives inputpower 256.

Wireless power transmission system 250 further includes one or morereceivers 260 coupled to or integrated within respective devices and arelocated at a distance from transmitter 252. Wireless power transmissionsystem 250 further includes an energy relay 270 including a relayantenna 272. As illustrated in FIG. 5A, the energy relay 270 operates asan intermediate energy relay between the transmitter 252 and thereceiver(s) 260, the coupling of which between the transmitter andreceiver(s) may be referred to as “vicinity” coupling.

In operation, transmitter 252 functions as an “exciter” of energy relay270 resulting generation of a magnetic near-field around the relayantenna 272. The magnetic near-field of energy relay 270 then couples toreceive antenna(s) 262 of receiver(s) 260. Accordingly, intermediateenergy relay 270 facilitates the transfer of the energy exhibited at thetransmit antenna 254 to effectively be received at the receiverantenna(s) 262. By way of example, a typical Q-value for energy relay270 may be on the order of Q-value of between 300 and 800.

FIG. 5B illustrates a configuration of wireless power transmissionsystem including an encompassing energy relay, in accordance with anexemplary embodiment. A wireless power transmission system 280 includesa transmitter 282 illustrated as a SDCP. The transmitter 282 furtherincludes a transmit antenna 284 and the transmitter 282 receives inputpower 286.

Wireless power transmission system 280 further includes one or morereceivers 290 coupled to or integrated within respective devices and arelocated at a distance from transmitter 282. Wireless power transmissionsystem 280 further includes an energy relay 300 including a relayantenna 302. As illustrated in FIG. 5B, the energy relay 300 operates asan intermediate energy relay between the transmitter 282 and thereceiver(s) 290, the coupling of which between the transmitter andreceiver(s) may also be referred to as “vicinity” coupling.

In operation, transmitter 282 functions as an “exciter” of energy relay300 generation of a magnetic near-field around the relay antenna 302.The magnetic near-field of energy relay 300 then couples to receiveantenna(s) 292 of receiver(s) 290. Accordingly, intermediate energyrelay 300 facilitates the transfer of the energy exhibited at thetransmit antenna 284 to effectively be received at the receiverantenna(s) 292. By way of example, a typical Q-value for energy relay300 may be on the order of Q-value of between 300 and 800.

FIG. 6 illustrates a device configured to receive wirelessly transmittedpower and to transmit wireless power, in accordance with an exemplaryembodiment. A device 400 includes a transmitter 104 and a receiver 108described above with respect to FIG. 2. Device 400 further includes atransmit/receive antenna 416 switchable according to switch 418 betweentransmitter 104 and receiver 108 for an exemplary embodiment where areceiver may be reconfigurable to operate as a transmitter to yetanother receiver. Furthermore, device 400 further includes a battery 136which is switchably coupled according to switch 420 to receive chargefrom receiver 108 or to provide input power 102 to transmitter 104.

In operation as a receiver, device 400 may be configured to receivewirelessly transmitted power from a separate transmitter (not shown) andstore the wirelessly receive power in battery 136 during deviceoperation as a receiver. In operation as a transmitter, device 400 maybe configured to generate a magnetic near-field using energy stored inbattery 136 as the input power 102.

FIG. 7 illustrates a wired power transmission system. A wired powertransmission system 500 includes AC input power, I_(AC), V_(AC),operating at an AC frequency, f_(AC). The input power is input into anAC-to-DC converter 502 operating at a switching frequency, f_(SW). A DCcord 504 runs the DC power, V_(DCL), I_(DCL), to device 506 while aswitch 508 selectively runs the input power to a battery 510.

A transmission efficiency may be calculated wherein the AC input power,P_(ACin), is defined as,

${P_{ACin} = {\frac{1}{T_{A\; C}}{\int_{0}^{T_{A\; C}}{{{v_{A\; C}(t)} \cdot {i_{A\; C}(t)}}\ {t}}}}};$$T_{A\; C} = \frac{1}{f_{A\; C}}$

and the DC input power, P′_(DCL), at the device input charging terminalsis defined as,

${P_{DCL}^{\prime} = {\frac{1}{T_{sw}}{\int_{0}^{T_{sw}}{{{v_{DCL}^{\prime}(t)} \cdot {i_{DCL}^{\prime}(t)}}\ {t}}}}};$$T_{sw} = \frac{1}{f_{sw}}$

while the DC input power, P_(DCL), at the battery terminals is definedas,

${P_{DCL} = {\frac{1}{T_{sw}}{\int_{0}^{T_{sw}}{{{v_{DCL}(t)} \cdot {i_{DCL}(t)}}\ {t}}}}};$$T_{sw} = {\frac{1}{f_{sw}}.}$

Therefore, efficiency as defined at the device terminals is defined as,

$\begin{matrix}{\eta^{\prime} = \frac{P_{DCL}^{\prime}}{P_{ACin}}} & \;\end{matrix}$

and overall (end-to-end) efficiency is defined as,

$\eta = \frac{P_{DCL}}{P_{ACin}}$

while a typical measured efficiency is around 60%-70%.

FIG. 8 illustrates a functional block diagram of a wireless powertransmission system, in accordance with various exemplary embodiments.Various ports are identified in FIG. 8, including input port 602 andoutput port 610, for comparison in subsequent figures illustratingcoupling variations. Wireless power transmission system 600 includes atransmitter 604 and a receiver 608. Input power P_(TXin) is provided totransmitter 604 for generating a predominantly non-radiative field withcoupling k 606 for providing energy transfer. Receiver 608 couples tothe non-radiative field 606 and generates an output power P_(PXout) forstoring or consumption by a battery or load 636 coupled to the outputport 610. Both the transmitter 604 and the receiver 608 are separated bya distance. In one exemplary embodiment, transmitter 604 and receiver608 are configured according to a mutual resonant relationship and whenthe resonant frequency, f₀, of receiver 608 and the resonant frequencyof transmitter 604 are matched, transmission losses between thetransmitter 604 and the receiver 608 are minimal while the receiver 608is located in the “near-field” of the radiated field 606.

Transmitter 604 further includes a transmit antenna 614 for providing ameans for energy transmission and receiver 608 further includes areceive antenna 618 for providing a means for energy reception.Transmitter 604 further includes a transmit power conversion unit 620 atleast partially function as an AC-to-AC converter. Receiver 608 furtherincludes a receive power conversion unit 622 at least partiallyfunctioning as an AC-to-DC converter. Various internal port currents,voltages and power are identified in FIG. 8 for comparison of variouscoupling variants in subsequent figures.

FIG. 9 illustrates a circuit diagram of a first coupling variant betweentransmit and receive antennas, in accordance with an exemplaryembodiment. The coupling variant 630 of FIG. 9 illustrates a “proximity”coupling variant finding application, for example, in a Single DeviceCharging Pad (SDCP) 200 of FIGS. 4A-4C. Coupling variant 630 includescoupled series tank circuits illustrated as a transmit antenna 614′ anda receive antenna 618′. Transmit antenna 614′ includes a series tankcircuit comprised of capacitor C₁ and inductor L₁ and receive antenna618′ includes another series tank circuit comprised of capacitor C₂ andinductor L₂.

Coupled series tank circuits generally do not exhibit detuning effectsif the coupling factor k₁₂ and/or the receiver load (not shown) ischanged. Moreover, a series tank circuit with open terminalstheoretically does not absorb energy in close proximity of atransmitter, which is in contrast to other coupling variants containinga parallel L-C structure that may absorb relatively high amounts ofpower independent of the loading at the receive terminals. Accordingly,coupling variant 630 of coupled series tanks provides efficient wirelesspower transmission for a single or multiple receiver configuration suchas is illustrated with respect to FIGS. 4A-4C.

FIG. 10 illustrates a circuit diagram of a second coupling variantbetween transmit and receive antennas, in accordance with an exemplaryembodiment. The coupling variant 650 of FIG. 10 illustrates a “vicinity”coupling variant and may be used to couple to a high-Q resonant tankcircuit used for “vicinity” coupling. Coupling variant 650 transformsimpedances to match with power conversion circuitry resulting in animproved or high transfer efficiency. Specifically, coupling variant 650includes a resonant transmit antenna 614″ and a resonant receive antenna618″.

Transmit antenna 614″ includes a high-Q tank resonator 652, includingcapacitor C₁ and inductor L₁, and a coupling loop/coil 654. Couplingloop/coil 654 matches the other portions of the transmitter to thehigh-Q tank resonator 652. Receive antenna 618″ includes a high-Q tankresonator 656, including capacitor C₂ and inductor L₂, and a couplingloop/coil 658. Coupling loop/coil 658 matches the other portions of thereceiver to the high-Q tank resonator 656.

FIG. 11 illustrates a circuit diagram of a third coupling variantbetween transmit and receive antennas, in accordance with an exemplaryembodiment. The coupling variant 670 uses capacitive coupling instead ofinductive coupling to transform the high impedance of high-Q paralleltank to match with transmit and receive power conversion units of FIG.8. Specifically, coupling variant 670 includes a transmit antenna 614′″and a receive antenna 618″′.

Transmit antenna 614″′ includes a high-Q parallel tank resonator 672,including capacitor C₁ and inductor L₁, and a coupling capacitor 674.Coupling capacitor 674 matches the other portions of the transmitter tothe high-Q parallel tank resonator 672. Receive antenna 618″′ includes ahigh-Q parallel tank resonator 676, including capacitor C₂ and inductorL₂, and a coupling capacitor 678. Coupling capacitor 678 matches theother portions of the receiver to the high-Q parallel tank resonator676.

FIG. 12 illustrates a circuit diagram of a fourth coupling variantbetween transmit and receive antennas, in accordance with an exemplaryembodiment. The coupling variant 690 uses a hybrid configuration ofseries and parallel tank circuits which may provide specific advantagesin some exemplary embodiments with regard to impedance matching oftransmit or receive power conversion. Specifically, coupling variant 690includes a transmit antenna 614″″ and a receive antenna 618″″.

Transmit antenna 614″″ may be configured similarly to transmit antenna614′ of FIG. 9. Transmit antenna 614″″ includes a series tank resonator692, including capacitor C₁ and inductor L₁ and receive antenna 618″″includes a parallel tank resonator 696, including capacitor C₂ andinductor L₂.

FIG. 13 illustrates a circuit diagram of a fifth coupling variantbetween transmit and receive antennas, in accordance with an exemplaryembodiment. The coupling variant 700 of FIG. 13 illustrates anembodiment for extending a system that is generally designed for“proximity” coupling using series resonant circuits for “vicinity”coupling. Coupling variant 700 includes a transmit antenna 614″″′ and areceive antenna 618′″″. Transmit antenna 614″″′ includes series tankresonator 704, including capacitor C₁ and inductor L₁ and receiveantenna 618″″′ includes a series tank resonator 706, including capacitorC₂ and inductor L₂. Transmit antenna 614″″′ and receive antenna 618″″′may also include one or more parasitic high-Q resonators 702.

In coupling variant 700, a parasitic high-Q resonator 702 is added aseither a parasitic high-Q resonator 702A in the transmit antenna 614″″′,a parasitic high-Q resonator 702B in the receive antenna 618″″′, orparasitic high-Q resonators 702A, 702B in both transmit antenna 614″″′and receive antenna 618″″′. Furthermore, matching can be controlled bychanging the coupling factors k_(11′) and/or k_(22′). By way of example,a typical Q-value for parasitic high-Q resonator 702A may be on theorder of a Q-value greater than 300 and the Q-value for parasitic high-Qresonator 702B may be on the order of a Q-value between 80 and 200.

Parasitic tanks may also be used for impedance conditioning at inputport 602 (FIG. 8) and the output port 610 (FIG. 8) of the couplingvariants in case the coupling factor k₁₂ would vary due to devicepositioning. Specifically, impedance as seen at input port 602 and theoptimum load impedance at the output port 610 may dramatically change,if the coupling factor k₁₂ varies, causing a need for impedanceadaptation on both sides of the power transfer link usually accomplishedby the transmit and receive power converters 620, 622 (FIG. 8). The useof a parasitic tank with a fixed coupling to its series tank (k_(11′))may stabilize this impedance to some degree while relaxing requirementsto the transmit and receive power conversion units 620, 622.

Generally, resonant antenna systems are subject of detuning effects fromextraneous objects. A receive antenna is typically detuned whenintegrated into a host device, due to effects of the device's body onmagnetic and electric fields. This effect can be accounted for by designand component selection. This is in contrast to a transmit antenna whosedetuning may be variable depending on the position of the device.Additionally, the unloaded Q-factor generally will drop due to eddycurrent losses and dielectric losses in the device's body.

As far as close “proximity” coupling is concerned, tuning of theantennas' resonance frequency may be less necessary, since resonantantennas will likely be highly loaded (i.e., low loaded Q-factors). Thismay be different in a system designed for “vicinity” coupling, where theoperational Q-factors will likely be high, thus requiring compensationfor any detuning effects. Furthermore, Q-drop by losses in the devicecannot be compensated for but has to be accepted. Depending on thesolution, it can affect both transmitter and receiver.

As stated above with reference to FIGS. 8-13, a wireless powertransmission system 600 includes a transmitter 604 and a receiver 608 asillustrated in FIG. 8. Wireless power transmission systems may beconfigured to operate at various resonant frequencies including “low”and “high” frequencies. An example of a low and high frequencyembodiments are described. A low frequency (LF) embodiment is describedwhere the transmit frequency, f₀=135 kHz (LF ISM-band for RFID systems).A high frequency (HF) embodiment is described where the transmitfrequency, f₀=13.56 MHz (HF ISM-band for RFID systems). In the followingfigures, difference between LF and HF systems are identified.

Regarding a transmitter, a low frequency or a high frequency (LF-HF)transmitter is comprised of two main parts, (1) a transmit powerconversion unit and (2) a transmit antenna (coupling unit). The transmitantenna basically consists of a loop/coil antenna and the anti-reactor(capacitor) to get the system on resonance.

FIG. 14 illustrates an LF-HF transmitter, in accordance with anexemplary embodiment. An LF-HF transmitter 800 includes a transmitantenna 802 illustrated as a series resonant tank circuit 804 includingcapacitor C₁ and inductor L₁. FIG. 14 also illustrates an equivalentresistor 806 representing the antenna's internal losses and externallosses due to the resonance dampening effect of objects in the antenna'sneighborhood. LF-HF transmitter 800 further includes a transmit powerconversion unit 808 comprised of an AC-to-AC converter subunit 810, afrequency generation & control subunit 812 and an auxiliary converter814 for supplying power to the frequency generation & control subunit812.

FIGS. 15A-15C illustrate various configurations of multiple stagetransmit power conversion units, in accordance with exemplaryembodiments. FIG. 15A illustrates a generalized two-stage exemplaryembodiment of an LF-HF transmit power conversion unit for generatingLF-HF power which includes a AC-to-DC conversion in a first stagefollowed by an LF-HF power stage. An LF-HF transmit power conversionunit 808A includes an AC-to-DC converter 820 with a variable outputpower and an LF-HF power stage 822 driven by the frequency generator(not shown) forming part of the frequency generation & control subunit812. An auxiliary converter 814 provides supply power at a generallylower and fixed voltage. One benefit of a double stage approach of FIG.15A is the variable DC supply of the power stage that can be used tocontrol power (P_(TXout)) into the coupling network.

FIG. 15B illustrates an exemplary embodiment of an LF-HF transmit powerconversion unit for generating LF-HF power which includes a half bridgeinverter power stage. An LF-HF transmit power conversion unit 808A′includes two FET switches 830A, 830B in configuration forming a halfbridge inverter 832. Desirably, to achieve high efficiency, the halfbridge inverter 832 switches at voltage/current zero crossings.Therefore, the duty cycle, for example, for LF having a f₀=135 kHz gatedrive waveform and HF having a f₀=13.56 MHz gate drive waveform is fixedaround 50%. Power control is accomplished by a DC-to-DC converter 834providing a PWM controlled variable output voltage V_(DC1). A 50% dutycycle also minimizes harmonic content. Nevertheless, additional PWMcontrol of the half bridge inverter 832 may be useful in some cases.

The DC-to-DC converter 834 may be switched at the operating frequency orat a different frequency (e.g. 200 kHz or higher) adjusted to therequirements. A conditioning network 836 at the output of the transmitpower conversion unit 808A′ may serve to suppress harmonics and/orincrease efficiency, depending on the coupling network. In the presentexemplary embodiment, while multiple FET switches 830 may be required,there is typically less voltage stress for the FETs compared to singleFET power stages, thus lower cost devices may be used. Furthermore, inthe present exemplary embodiment, the half bridge inverter power stageoperates like a voltage source (low impedance) and thus may drive anyload impedance as long as currents and/or power do not exceed FETratings. The half bridge inverter is particularly suitable to driveseries resonant tanks.

FIG. 15C illustrates another exemplary embodiment of an LF-HF transmitpower conversion unit for generating LF-HF power which includes a ‘boostconverter’-like or class E configured power stage. LF-HF transmit powerconversion unit 808A″ includes one FET switch 830 configured to form a‘boost converter’-like or class E circuit, with the FET switch “on-time”occurring at zero volts (class E or soft switching approach).

If the LF-HF transmit power conversion unit is to drive a transmitantenna configured as a series resonant tank, this series resonant tankthen functions as part of a series C-L-R_(L) load network typicallyutilized for class E operation. The gate drive may be additional PWMcontrolled for impedance matching or power control purposes. Generally,the highest efficiency is achieved at 50% duty cycle. A DC-to-DC stepdown converter 842 may be switched at the operating frequency or at adifferent frequency (e.g. 200 kHz or higher) adjusted to therequirements. A conditioning network 844 at the output of the transmitpower conversion unit 808A″ may serve to suppress harmonics and/orincrease efficiency and matching, depending on the coupling network.

FIGS. 16A-16D illustrate various configurations of single stage transmitpower conversion units, in accordance with exemplary embodiments.Generation of LF-HF power directly from the main AC voltage using asingle stage approach is illustrated in FIG. 16A. Since DC supplyvoltage may be fixed and high (e.g., in the range 120-315 VDC), powercontrol can be accomplished by means of the duty cycle of the switchingwaveform (PWM). In this approach, the AC-to-AC converter 850 may beconsidered as a part of a transformer isolated AC-to-DC power supply.The coupling network acts as an isolation transformer but with highleakage or stray inductance. The transmit power conversion unit 808Bfurther includes of a frequency generation & control subunit 812 and anauxiliary converter 814 for supplying power to the frequency generation& control subunit 812.

FIG. 16B illustrates an exemplary embodiment of an LF-HF transmit powerconversion unit for generating LF-HF power. LF-HF transmit powerconversion unit 808W includes one FET switch 830 and the output powercontrol in LF-HF transmit power conversion unit 808B′ is accomplishedusing a PWM gate driving waveform of f₀=135 kHz for LF and f₀=13.56 MHzfor HF, meaning that efficiency may be somewhat compromised at low dutycycles (i.e., conduction angle). However, the duty cycle needed toachieve the target power can be increased by designing the couplingnetwork with a transformation ratio n:1 (n>1), meaning that a highprimary voltage is transformed to a low secondary voltage.

If the LF-HF transmit power conversion unit is to drive a transmitantenna configured as a series resonant tank, this series resonant tankthen functions as part of a series C-L-R_(L) load network typicallyutilized for class E operation. A conditioning network 844 at the outputof the transmit power conversion unit 808B′ may serve to suppressharmonics and/or increase efficiency and matching, depending on thecoupling network. This may be of particular importance for the PWMapproach, since harmonic content increases with decreasing duty cycle.

FIG. 16C illustrates another exemplary embodiment of an LF-HF transmitpower conversion unit for generating LF-HF power. LF-HF transmit powerconversion unit 808B″ includes one FET switch 830 forming the powerstage. The resonant tank circuit 804 of the transmit antenna 802 is‘suspended’ between the DC supply voltage and ground with the powerstage connected to the ‘hot end’ of the resulting tank circuit.

FIG. 16D illustrates another exemplary embodiment of an LF-HF transmitpower conversion unit for generating LF-HF power. LF-HF transmit powerconversion unit 808B″′ includes a FET switch 830 operating in series toa shunt inductance, inductor 852. LF-HF transmit power conversion unit808B″′ may drive a transmit antenna 802 configured as a series resonanttank.

Regarding a receiver, an LF-HF receiver is comprised of two main parts,(1) a receive antenna (coupling unit) and (2) a receive power conversionunit. The receive antenna basically consists of a loop/coil antenna andthe anti-reactor (capacitor) to get the system on resonance.

FIG. 17 illustrates an LF-HF receiver, in accordance with an exemplaryembodiment. An LF-HF receiver 900 includes a receive antenna 902illustrated as a series resonant tank circuit 904 including capacitor C₂and inductor L₂. FIG. 17 also illustrates an equivalent resistor 906representing the antenna's internal losses and external losses due tothe resonance dampening effect of objects in the antenna's neighborhood.LF-HF receiver 900 further includes a receive power conversion unit 908comprised of an AC-to-DC converter subunit 910 and a frequencygeneration & control subunit 912. FIG. 17 further illustrates LF-HFreceiver 900 coupling to a load 916 of the device.

Generally, the various above descriptions of the transmit antenna 802also find application to receive antenna 902. The power required tosupply the frequency generation & control subunit 912 may be receivedfrom the receive power conversion unit 908. In one exemplary embodiment,the receive power conversion unit 908 operates in a “minimum mode” bygenerating sufficient power to feed the frequency generation & controlsubunit 912 independently of any ability of the load 916 (e.g., battery)to source power to the receive power conversion unit 908, provided powerreceived from the receive antenna exceeds a threshold. Once thefrequency generation & control unit 908 is fully operational, thereceive power conversion unit 908 enters a “normal mode” and deliverspower to the load 916.

In receive power conversion unit 908, frequencies may be required forDC-to-DC conversion and/or for synchronous rectification. With asynchronous rectifier, power flow may be reversed such that the receiveracts as a power transmitter. In the minimum mode, the AC-to-DC converter910 performs as a passive diode rectifier with additional components tosense charging voltage and current and a switch (not shown) todisconnect the load 916 (e.g., battery). FIG. 17 also illustrates portsand interfaces and designates port currents, voltages and powers.

FIGS. 18A-18H illustrate various configurations of receive powerconversion units, in accordance with various exemplary embodiments. FIG.18 A illustrates a receive power conversion unit, in accordance with anexemplary embodiment. LF-HF receive power conversion unit 908A includesan AC rectifier 920 and a DC-to-DC converter unit 922. DC-to-DCconverter unit 922 is used to adjust load impedance as seen by thecoupling network at the input port of AC rectifier 920 in order tomaximize transfer efficiency. In various load ranges, efficiency doesnot alter significantly if the load impedance is changed. Receive loadimpedance control may also be used to condition the impedance at thetransmit port of the coupling network.

FIG. 18B illustrates another exemplary embodiment of an LF-HF receivepower conversion unit. LF-HF receive power conversion unit 908A′includes a quad diode full wave full bridge rectifier 920′ and DC-to-DCconverter unit 922′. Furthermore, rectifier structure variations ofrectifier 920 are also contemplated.

In various practical applications, the load 916 (e.g., battery) has lowvoltage (e.g. 4 V) and high current (e.g. 1 A) thus imposing a lowresistance low (e.g. 4 ohms) requiring a step down converter.Accordingly, the use of a DC-to-DC converter is particularlyadvantageous, since a DC-to-DC converter allows rectifier 920 to beoperated at higher input voltages V_(A2) where a diode's thresholdvoltages have less impact, thus increasing the efficiency of rectifier920. Theoretically, the DC-to-DC step down-converter 922′ may switch ata different frequency that is determined to achieve maximum efficiency.The load current can be regulated by means of the duty cycle of the PWMswitching waveform.

FIG. 18C illustrates another exemplary embodiment of an LF-HF receivepower conversion unit. LF-HF receive power conversion unit 908B is basedon synchronous rectification, meaning that active FET switches (notshown) are used to rectify the received LF-HF power. The switchingwaveform must be synchronous to the received signal and the waveform'sphase must be adjusted. Adjustment may be accomplished using avoltage/current sense.

The frequency generation and control unit 912 generates the switchingwaveforms and may perform load power and impedance control by means ofPWM. In this exemplary embodiment, the AC-to-DC converter 924 may beconsidered as the secondary part of a transformer-isolated AC-to-DCpower supply. The coupling network acts as an isolation transformer butwith high leakage or stray inductance.

FIG. 18D illustrates exemplary embodiments of an AC-to-DC converter. Inthe exemplary embodiments, AC-to-DC converter 924A and AC-to-DCconverter 924B are configured to also perform synchronous rectificationaccording to a single FET synchronous rectifier 926. A clock recoveryand phase angle control 928 is required to properly align the FET drivewaveform to the received waveform, so that the synchronous rectifieroperates in the right V-I quadrant. These functions may be consideredpart of the frequency generation & control subunit 912. The FETsynchronous rectifier 926 may be operated with reduced/increased dutycycles to control the converters input impedance and power. AC-to-DCconverter 924A finds application with a parallel resonant tank in areceive antenna and AC-to-DC converter 924B finds application with aseries resonant tank in a receive antenna.

If AC-to-DC converter 924A couples to a series resonant tank in thereceive antenna, then a parallel capacitor C_(p2) 930 and switching atzero volts by the FET synchronous rectifier 926 may be needed to avoidFET switching stress. However, capacitor C_(p2) 930 tends to decreasethe converters input impedance, which may be counterproductive in astrongly coupled regime (transmitter and receiver in close proximity).If AC-to-DC converter 924B couples to a parallel resonant tank in thereceive antenna, then a series inductor L_(s2) 932 may be needed and theFET synchronous rectifier 926 should be opened only at zero current toavoid FET switching stress.

FIG. 18E illustrates another exemplary embodiment of an LF-HF receivepower conversion unit. LF-HF receive power conversion unit 908C is basedon a passive diode rectifier 934 and is considered particularly suitablefor very small form factor micro power devices, where ultimate transferefficiency may not be the primary issue. However, passive dioderectifiers normally may be difficult to control in terms of loadimpedance matching and output power. Thus the receiver should bedesigned and optimized to the coupling regime that is most probable inthe envisaged application or use case. A limited control may beincorporated all the same e.g. by changing the configuration of a dioderectifier using static FET switches. Diode rectifiers and rectifiers ingeneral may be categorized as shown:

Current sink Voltage sink Single diode (half wave) Type a Type b Doublediode (full wave, half bridge) Type c Type d Quad diode (full wave, fullbridge) Type e Type f

FIG. 18F illustrates exemplary embodiments of a passive diode rectifier.In the exemplary embodiments, passive diode rectifier 934A is a suitablestructure to cooperate with a parallel resonant tank in a receiveantenna. Passive diode rectifier 934A exhibits an input impedance whichis higher than its load impedance, thus performing voltage downconversion. Passive diode rectifier 934B is a suitable structure tocooperate with a series resonant tank in a receive antenna.

If the passive diode rectifier 934A couples to a series resonant tank inthe receive antenna, then a parallel capacitor C_(p2) 936 may be neededto avoid diode switching stress. However, capacitor C_(p2) 936 tends todecrease the converters input impedance, which may be counterproductivein a strongly coupled regime (i.e., transmitter and receiver in closeproximity). If the passive diode rectifier 934B couples to a parallelresonant tank in a receive antenna, then a series inductor L_(s2) 938may be needed to avoid diode switching stress.

FIG. 18G illustrates exemplary embodiments of a passive diode rectifier.In the exemplary embodiments, passive diode rectifiers 934C, 934D aredouble diode rectifiers. Passive diode rectifier 934C is a suitablestructure to cooperate with a parallel resonant tank in a receiveantenna. Passive diode rectifier 934C exhibits an input impedance whichis higher than its load impedance and higher than that achieved withpassive diode rectifier 934A. Passive diode rectifier 934D is the dualdiode structure to passive diode rectifier 934B, and more suitable to bedriven from a series resonant tank in a receive antenna. However,passive diode rectifier 934D exhibits a lower input impedance than itsload impedance and lower than that achieved with Passive diode rectifier934B.

If the passive diode rectifier 934C couples to a series resonant tank ina receive antenna, then a parallel capacitor C_(p2) 940 may be requiredto avoid diode switching stress (high dV/dt). However, parallelcapacitor C_(p2) 940 tends to decrease the converters input impedance,which may be counterproductive in a strongly coupled regime (transmitterand receiver in close proximity). If the passive diode rectifier 934Dcouples to a parallel resonant tank in a receive antenna, then a seriesinductor L_(s2) 942 may be needed to avoid diode switching stress (highdI/dt).

FIG. 18H illustrates exemplary embodiments of a passive diode rectifier.In the exemplary embodiments, passive diode rectifiers 934E, 934F arequad diode rectifiers and may be considered as pair of half bridge(Class D) rectifiers operated in ‘push-pull’ (anti-phase). Passive dioderectifier 934E operates as a current sink and is a suitable structure tocooperate with a parallel resonant tank in a receive antenna. Passivediode rectifier 934E exhibits an input impedance which is higher thanits load impedance and double of that achieved with passive dioderectifier 934C. Passive diode rectifier 934F operates as a voltage sinkand is the dual structure of passive diode rectifier 934D, thus moresuitable to be driven from a series resonant tank in a receive antenna.However, passive diode rectifier 934F exhibits a lower input impedancethan its load impedance but doubles that of passive diode rectifier934D, which is advantageous in a strongly coupled regime.

If the passive diode rectifier 934E couples to a series resonant tank ina receive antenna, then a parallel capacitor C_(p2) 944 may be requiredto avoid diode switching stress (high dV/dt). However, parallelcapacitor C_(p2) 944 tends to decrease the converters input impedance,which may be counterproductive in a strongly coupled regime (transmitterand receiver in close proximity). If the passive diode rectifier 934Fcouples to a parallel resonant tank in a receive antenna, then a seriesinductor L_(s2) 946 may be needed to avoid diode switching stress (highdI/dt).

FIG. 19 illustrates a flowchart of a method for receiving wirelesspower, in accordance with an exemplary embodiment. Method 1000 forreceiving wireless power is supported by the various structures andcircuits described herein. Method 1000 includes a step 1002 forreceiving at a series configured resonant tank of a receive antenna,wireless power in a magnetic near field generated by a transmit antennawhen the receive antenna and the transmit antenna are proximity coupled.The method 1000 further includes a step 1004 for receiving at a seriesconfigured resonant tank of a receive antenna, wireless power in amagnetic near field generated by a transmit antenna when the receiveantenna and the transmit antenna are proximity coupled. Furthermore, themethod 1000 further includes a step 1006 for receiving at a parasiticresonant tank of the receive antenna, the wireless power of the magneticnear field generated by the transmit antenna when the receive antennaand the transmit antenna are vicinity coupled. The method 1000 furtherincludes a step 1006 fore rectifying the wireless power.

FIG. 20 illustrates a flowchart of a method for transmitting wirelesspower, in accordance with an exemplary embodiment. Method 1100 fortransmitting wireless power is supported by the various structures andcircuits described herein. Method 1100 includes a step 1102 forgenerating at a series configured resonant tank of a transmit antennawireless power in a magnetic near field when a receive antenna and thetransmit antenna are proximity coupled. Method 1100 further includes astep 1104 for generating at a parasitic resonant tank of the transmitantenna the wireless power of the magnetic near field when the receiveantenna and the transmit antenna are vicinity coupled.

Those of skill in the art would understand that control information andsignals may be represented using any of a variety of differenttechnologies and techniques. For example, data, instructions, commands,information, signals, bits, symbols, and chips that may be referencedthroughout the above description may be represented by voltages,currents, electromagnetic waves, magnetic fields or particles, opticalfields or particles, or any combination thereof.

Those of skill would further appreciate that the various illustrativelogical blocks, modules, circuits, and algorithm steps described inconnection with the embodiments disclosed herein may be implemented aselectronic hardware, and controlled by computer software, orcombinations of both. To clearly illustrate this interchangeability ofhardware and software, various illustrative components, blocks, modules,circuits, and steps have been described above generally in terms oftheir functionality. Whether such functionality is implemented andcontrolled as hardware or software depends upon the particularapplication and design constraints imposed on the overall system.Skilled artisans may implement the described functionality in varyingways for each particular application, but such implementation decisionsshould not be interpreted as causing a departure from the scope of theexemplary embodiments of the invention.

The various illustrative logical blocks, modules, and circuits describedin connection with the embodiments disclosed herein may be controlledwith a general purpose processor, a Digital Signal Processor (DSP), anApplication Specific Integrated Circuit (ASIC), a Field ProgrammableGate Array (FPGA) or other programmable logic device, discrete gate ortransistor logic, discrete hardware components, or any combinationthereof designed to perform the functions described herein. A generalpurpose processor may be a microprocessor, but in the alternative, theprocessor may be any conventional processor, controller,microcontroller, or state machine. A processor may also be implementedas a combination of computing devices, e.g., a combination of a DSP anda microprocessor, a plurality of microprocessors, one or moremicroprocessors in conjunction with a DSP core, or any other suchconfiguration.

The control steps of a method or algorithm described in connection withthe embodiments disclosed herein may be embodied directly in hardware,in a software module executed by a processor, or in a combination of thetwo. A software module may reside in Random Access Memory (RAM), flashmemory, Read Only Memory (ROM), Electrically Programmable ROM (EPROM),Electrically Erasable Programmable ROM (EEPROM), registers, hard disk, aremovable disk, a CD-ROM, or any other form of storage medium known inthe art. An exemplary storage medium is coupled to the processor suchthat the processor can read information from, and write information to,the storage medium. In the alternative, the storage medium may beintegral to the processor. The processor and the storage medium mayreside in an ASIC. The ASIC may reside in a user terminal. In thealternative, the processor and the storage medium may reside as discretecomponents in a user terminal.

In one or more exemplary embodiments, the control functions describedmay be implemented in hardware, software, firmware, or any combinationthereof. If implemented in software, the functions may be stored on ortransmitted over as one or more instructions or code on acomputer-readable medium. Computer-readable media includes both computerstorage media and communication media including any medium thatfacilitates transfer of a computer program from one place to another. Astorage media may be any available media that can be accessed by acomputer. By way of example, and not limitation, such computer-readablemedia can comprise RAM, ROM, EEPROM, CD-ROM or other optical diskstorage, magnetic disk storage or other magnetic storage devices, or anyother medium that can be used to carry or store desired program code inthe form of instructions or data structures and that can be accessed bya computer. Also, any connection is properly termed a computer-readablemedium. For example, if the software is transmitted from a website,server, or other remote source using a coaxial cable, fiber optic cable,twisted pair, digital subscriber line (DSL), or wireless technologiessuch as infrared, radio, and microwave, then the coaxial cable, fiberoptic cable, twisted pair, DSL, or wireless technologies such asinfrared, radio, and microwave are included in the definition of medium.Disk and disc, as used herein, includes compact disc (CD), laser disc,optical disc, digital versatile disc (DVD), floppy disk and blu-ray discwhere disks usually reproduce data magnetically, while discs reproducedata optically with lasers. Combinations of the above should also beincluded within the scope of computer-readable media.

The previous description of the disclosed exemplary embodiments isprovided to enable any person skilled in the art to make or use thepresent invention. Various modifications to these exemplary embodimentswill be readily apparent to those skilled in the art, and the genericprinciples defined herein may be applied to other embodiments withoutdeparting from the spirit or scope of the invention. Thus, the presentinvention is not intended to be limited to the embodiments shown hereinbut is to be accorded the widest scope consistent with the principlesand novel features disclosed herein.

1. A wireless power receiver, comprising: a receive antenna configuredto receive wireless power from a magnetic near field, the receiveantenna including: a resonant tank; and a parasitic resonant tankwirelessly coupled to the resonant tank.
 2. The wireless power receiverof claim 1, wherein the resonant tank couples with the magnetic nearfield when the receive antenna is within a proximity that is less than afirst distance away from a transmitter generating the magnetic nearfield.
 3. The wireless power receiver of claim 2, wherein the parasiticresonant tank couples with the magnetic near field when the receiveantenna is within a vicinity that is greater than the distance away fromthe transmitter.
 4. The wireless power receiver of claim 3, wherein theparasitic resonant tank inductively couples received wireless power tothe series configured resonant tank.
 5. The wireless power receiver ofclaim 1, wherein the parasitic resonant tank is a high-Q resonatorhaving a Q-value greater than the resonant tank.
 6. A wireless powertransmitter, comprising: a transmit antenna configured to generate amagnetic near field for transmission of wireless power, the transmitantenna including; a resonant tank; and a parasitic resonant tankwirelessly coupled to the resonant tank.
 7. The wireless powertransmitter of claim 6, wherein the resonant tank generates the magneticnear field when the transmit antenna is within a proximity that is lessthan a first distance away from a receiver receiving the wireless powerfrom the magnetic near field.
 8. The wireless power transmitter of claim7, wherein the parasitic resonant tank generates the magnetic near fieldwhen the transmit antenna is within a vicinity that is greater than thedistance away from the receiver.
 9. The wireless power transmitter ofclaim 8, wherein the resonant tank inductively couples the wirelesspower to parasitic resonant tank.
 10. The wireless power transmitter ofclaim 6, wherein the parasitic resonant tank is a high-Q resonatorhaving a Q-value greater than the resonant tank.
 11. A wireless powertransmission system, comprising: a transmitter including a transmitantenna for generating a magnetic near field for transmission ofwireless power, the transmit antenna including a first resonant tank; areceiver including a receive antenna for coupling with the transmitantenna to receive the wireless power from the magnetic near field, thereceive antenna including a second resonant tank; and a first parasiticresonant tank wirelessly coupled to one of the first and second resonanttanks
 12. The wireless power transmission system of claim 11, furthercomprising a second parasitic resonant tank wirelessly coupled toanother one of the first and second resonant tanks.
 13. The wirelesspower transmission system of claim 12, wherein the first and secondresonant tanks are configured for the wireless power transmissiontherebetween when the transmit antenna is within a proximity that isless than a first distance away from the receive antenna.
 14. Thewireless power transmission system of claim 13, wherein the first andsecond parasitic resonant tanks are configured for the wireless powertransmission therebetween when the transmit antenna is within a vicinitythat is greater than the distance away from the receive antenna.
 15. Thewireless power transmission system of claim 11, wherein the one of thefirst and second resonant tanks inductively couples the wireless powerto the first parasitic resonant tank.
 16. A method for receivingwireless power, comprising: receiving at a resonant tank of a receiveantenna wireless power in a magnetic near field generated by a transmitantenna when the receive antenna and the transmit antenna are within aproximity that is less than a distance away; receiving at a parasiticresonant tank of the receive antenna the wireless power of the magneticnear field generated by the transmit antenna when the receive antennaand the transmit antenna are within a vicinity that is greater than thedistance away; and rectifying the wireless power.
 17. The method forreceiving wireless power of claim 16, further comprising inductivelycoupling the wireless power from the parasitic resonant tank to theresonant tank when the receive antenna and the transmit antenna arewithin the vicinity that is greater than the distance away.
 18. Themethod for receiving wireless power of claim 16, wherein the parasiticresonant tank is a high-Q resonator having a Q-value greater than theresonant tank.
 19. A method for transmitting wireless power, comprising:generating at a resonant tank of a transmit antenna wireless power in amagnetic near field when a receive antenna and the transmit antenna arewithin a proximity that is less than a distance away; and generating ata parasitic resonant tank of the transmit antenna the wireless power ofthe magnetic near field when the receive antenna and the transmitantenna are within a vicinity that is greater than the distance away.20. The method for transmitting wireless power of claim 19, furthercomprising inductively coupling the wireless power from the resonanttank to the parasitic resonant tank when the receive antenna and thetransmit antenna are within the vicinity that is greater than thedistance away.
 21. The method for transmitting wireless power of claim19, wherein the parasitic resonant tank is a high-Q resonator having aQ-value greater than the resonant tank.
 22. A wireless power receiver,comprising: means for receiving at a resonant tank of a receive antennawireless power in a magnetic near field generated by a transmit antennawhen the receive antenna and the transmit antenna are within a proximitythat is less than a distance away; means for receiving at a parasiticresonant tank of the receive antenna the wireless power of the magneticnear field generated by the transmit antenna when the receive antennaand the transmit antenna are within a vicinity that is greater than thedistance away; and means for rectifying the wireless power.
 23. Awireless power transmitter, comprising: means for generating at aresonant tank of a transmit antenna wireless power in a magnetic nearfield when a receive antenna and the transmit antenna are within aproximity that is less than a distance away; and means for generating ata parasitic resonant tank of the transmit antenna the wireless power ofthe magnetic near field when the receive antenna and the transmitantenna are within a vicinity that is greater than the distance away.